Published June 16, 2022 | Version v1
Dataset Open

Enhancement of exchange bias and perpendicular magnetic anisotropy in CoO/Co multilayer thin films by tuning the alumina template nanohole size

  • 1. Departamento de Física Aplicada, EIG, Universidad del País Vasco, UPV/EHU, 20018, San Sebastián, Spain.
  • 2. Chemistry Department, College of Science, King Saud University, Riyadh, 11451, Saudi Arabia
  • 3. Chemistry Department, Faculty of Science, Sohag University, 82524, Sohag, Egypt
  • 4. Departamento de Física, Universidad de Oviedo, C/ Federico García Lorca 18, 33007 Oviedo, Asturias, Spain.
  • 5. Instituto Regional de Investigación Científica Aplicada (IRICA), Universidad de Castilla-La Mancha, 13071 Ciudad Real, Spain.

* Contact person

Description

The interest in magnetic nanostructures exhibiting perpendicular magnetic anisotropy and ex-change bias effect has increased in recent years owing to their applications in a new generation of spintronic devices that combine several functionalities. We present a nanofabrication process used to induce perpendicular magnetic anisotropy and exchange bias. 30-nm-thick CoO/Co multilayers were deposited on nanostructured alumina templates with a broad range of pore diameters, 34 nm ≤ Dp ≤ 96 nm, while maintaining the hexagonal lattice parameter at 107 nm. Increase of both the exchange bias field (HEB) and the coercivity (HC) (12 times and 27 times, respectively) was ob-served in the nanostructured films compared to the non-patterned film. The marked dependence of HEB and HC with antidot hole diameters pinpoints to an in-plane to out-of-plane changeover of the magnetic anisotropy at a nanohole diameter of ∼ 75 nm. Micromagnetic simulation shows the existence of antiferromagnetic layers that generate an exceptional magnetic configuration around the holes, named as antivortex-state. This configuration is responsible of inducing extra high-energy superdomain walls for samples with edge-to-edge distance (W) >> 27 nm and high-energy stripe magnetic domains for W < 27 nm, responsible of the perpendicular magnetic signal of the samples.

Files

File preview

files_description.md

All files

Files (1.3 MiB)

Name Size
md5:aeb8a69d757c87eccddeee56dad49711
1.5 KiB Preview Download
md5:4df33144a5bd1c7b209e7a8e0526d0d3
15.2 KiB Download
md5:f9b63b3ce599e55b4931909ab5fcdf7d
208.0 KiB Download
md5:b44475c51b23b8e54dd1800970b6d7ca
113.6 KiB Download
md5:3b2a598106c8ebc3ad0c15890c9af238
128 Bytes Download
md5:5f3ebf0af7db67f25d3a80776db8b55d
40.5 KiB Download
md5:29ec0bc9ed429fc99a6e5a31f87edd81
49.7 KiB Download
md5:0903292c6ff3a46854dae2ed931cfc2f
410.1 KiB Preview Download
md5:c475d0e93866232594072492c628d935
518.9 KiB Preview Download

References

Journal reference (Paper in which the data is discussed)
Mohamed Salaheldeen, Ayman Nafady, Ahmed M. Abu-Dief, Rosario Díaz Crespo, María Paz Fernández-García, Juan Pedro Andrés, Ricardo López Antón, Jesús A. Blanco, Pablo Álvarez-Alonso. Submitted to Nanomaterials